In a Young’s double slit experiment, the slit separation is 0.2 cm, the distance between the screen and slit is 1m. Wavelength of the light used is 5000 Å. The distance between two consecutive dark fringes (in mm) is
(1) 0.25
(2) 0.26
(3) 0.27
(4) 0.28
A slit of width a is illuminated by white light. For red light (λ = 6500 Å), the first minima is obtained at θ = 30°. Then the value of a will be
(1) 3250 Å
(2) 6.5 × 10–4 mm
(3) 1.24 microns
(4) 2.6 × 10–4 cm
What will be the angular width of central maxima in Fraunhoffer diffraction when light of wavelength is used and slit width is 12×10–5 cm
(1) 2 rad
(2) 3 rad
(3) 1 rad
(4) 8 rad
A beam of light of wavelength 600 nm from a distant source falls on a single slit 1 mm wide and the resulting diffraction pattern is observed on a screen 2 m away. The distance between the first dark fringes on either side of the central bright fringe is
(1) 1.2 mm
(2) 1.2 cm
(3) 2.4 cm
(4) 2.4 mm
Direction of the first secondary maximum in the Fraunhofer diffraction pattern at a single slit is given by (a is the width of the slit)
(1)
(2)
(3)
(4)
A parallel monochromatic beam of light is incident normally on a narrow slit. A diffraction pattern is formed on a screen placed perpendicular to the direction of the incident beam. At the first minimum of the diffraction pattern, the phase difference between the rays coming from the edges of the slit is
(1)
(2)
(3)
(4) 2
A parallel beam of monochromatic light of wavelength 5000 Å is incident normally on a single narrow slit of width 0.001 mm. The light is focused by a convex lens on a screen placed on the focal plane. The first minimum will be formed for the angle of diffraction equal to
(1) 0o
(2) 15o
(3) 30o
(4) 60o
In the far field diffraction pattern of a single slit under polychromatic illumination, the first minimum with the wavelength is found to be coincident with the third maximum at . So
(1)
(2)
(3)
(4)
A beam of light \(AO\) is incident on a glass slab \((\mu= 1.54)\) in a direction as shown in the figure. The reflected ray \(OB\) is passed through a Nicol prism. On viewing through a Nicole prism, we find on rotating the prism that:
1. | the intensity is reduced down to zero and remains zero. |
2. | the intensity reduces down somewhat and rises again. |
3. | there is no change in intensity. |
4. | the intensity gradually reduces to zero and then again increases. |